Search results for "Accelerator physics"

showing 10 items of 1294 documents

Operation and characterization of a windowless gas jet target in high-intensity electron beams

2021

Abstract A cryogenic supersonic gas jet target was developed for the MAGIX experiment at the high-intensity electron accelerator MESA. It will be operated as an internal, windowless target in the energy-recovering recirculation arc of the accelerator with different target gases, e.g., hydrogen, deuterium , helium, oxygen, argon, or xenon. Detailed studies have been carried out at the existing A1 multi-spectrometer facility at the electron accelerator MAMI. This paper focuses on the developed handling procedures and diagnostic tools, and on the performance of the gas jet target under beam conditions. Considering the special features of this type of target, it proves to be well suited for a n…

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsNuclear engineeringchemistry.chemical_elementFOS: Physical sciencesElectron01 natural scienceslaw.inventionXenonlaw0103 physical sciencesNuclear Experiment (nucl-ex)010306 general physicsInstrumentationNuclear ExperimentHeliumPhysicsJet (fluid)Argon010308 nuclear & particles physicsParticle acceleratorInstrumentation and Detectors (physics.ins-det)chemistryPhysics::Accelerator PhysicsElectron scatteringBeam (structure)
researchProduct

Coherent elastic neutrino-nucleus scattering at the European Spallation Source

2020

The European Spallation Source (ESS), presently well on its way to completion, will soon provide the most intense neutron beams for multi-disciplinary science. Fortuitously, it will also generate the largest pulsed neutrino flux suitable for the detection of Coherent Elastic Neutrino-Nucleus Scattering (CE$\nu$NS), a process recently measured for the first time at ORNL's Spallation Neutron Source. We describe innovative detector technologies maximally able to profit from the order-of-magnitude increase in neutrino flux provided by the ESS, along with their sensitivity to a rich particle physics phenomenology accessible through high-statistics, precision CE$\nu$NS measurements.

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaFluxFOS: Physical sciences01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesElectroweak interactionlcsh:Nuclear and particle physics. Atomic energy. RadioactivityNeutronSpallationNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentPhysics010308 nuclear & particles physicsScatteringElectroweak interactionDetectorInstrumentation and Detectors (physics.ins-det)Neutrino Detectors and Telescopes (experiments)High Energy Physics - PhenomenologyBeyond Standard Modellcsh:QC770-798Physics::Accelerator PhysicsNeutrinoSpallation Neutron Source
researchProduct

The ATLAS level-1 trigger: Status of the system and first results from cosmic-ray data

2007

The ATLAS detector at CERN's Large Hadron Collider (LHC) will be exposed to proton-proton collisions from beams crossing at 40 MHz. At the design luminosity of 10^34 cm^-2 s^-1 there are on average 23 collisions per bunch crossing. A three-level trigger system will select potentially interesting events in order to reduce the read-out rate to about 200 Hz. The first trigger level is implemented in custom-built electronics and makes an initial fast selection based on detector data of coarse granularity. It has to reduce the rate by a factor of 10^4 to less than 100 kHz. The other two consecutive trigger levels are in software and run on PC farms. We present an overview of the first-level trig…

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsPhysics::Instrumentation and DetectorsAtlas detectoratlas; cosmic-ray data; installation and commissioning; trigger systemFOS: Physical sciencesCosmic rayinstallation and commissioningNuclear physicsSoftwareAtlas (anatomy)medicineatlascosmic-ray dataDetectors and Experimental TechniquesInstrumentationPhysicstrigger systemLarge Hadron ColliderLuminosity (scattering theory)business.industrySettore FIS/01 - Fisica SperimentaleDetectorInstrumentation and Detectors (physics.ins-det)medicine.anatomical_structurePhysics::Accelerator PhysicsGranularitybusinessNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
researchProduct

High-gradient testing of an $S$-band, normal-conducting low phase velocity accelerating structure

2020

A novel high-gradient accelerating structure with low phase velocity, $v/c=0.38$, has been designed, manufactured and high-power tested. The structure was designed and built using the methodology and technology developed for CLIC $100\text{ }\text{ }\mathrm{MV}/\mathrm{m}$ high-gradient accelerating structures, which have speed of light phase velocity, but adapts them to a structure for nonrelativistic particles. The parameters of the structure were optimized for the compact proton therapy linac project, and specifically to 76 MeV energy protons, but the type of structure opens more generally the possibility of compact low phase velocity linacs. The structure operates in S-band, is backward…

Nuclear and High Energy PhysicsPhysics and Astronomy (miscellaneous)Field (physics)[PHYS.PHYS.PHYS-ACC-PH]Physics [physics]/Physics [physics]/Accelerator Physics [physics.acc-ph]cavityType (model theory)01 natural sciencesp: accelerationLinear particle accelerator0103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsReview ArticlesPhysics010308 nuclear & particles physicsvelocity: lowPulse durationSurfaces and Interfaceslinear acceleratorgradient: highAccelerators and Storage Ringsvelocity: phasePulse (physics)particle: nonrelativisticDistribution (mathematics)lcsh:QC770-798Atomic physicsPhase velocityEnergy (signal processing)performance
researchProduct

High intensity neutrino oscillation facilities in Europe

2013

The EUROnu project has studied three possible options for future, high intensity neutrino oscillation facilities in Europe. The first is a Super Beam, in which the neutrinos come from the decay of pions created by bombarding targets with a 4 MW proton beam from the CERN High Power Superconducting Proton Linac. The far detector for this facility is the 500 kt MEMPHYS water Cherenkov, located in the Frejus tunnel. The second facility is the Neutrino Factory, in which the neutrinos come from the decay of mu(+) and mu(-) beams in a storage ring. The far detector in this case is a 100 kt magnetized iron neutrino detector at a baseline of 2000 km. The third option is a Beta Beam, in which the neu…

Nuclear and High Energy PhysicsPhysics and Astronomy (miscellaneous)Physics::Instrumentation and Detectors[PHYS.PHYS.PHYS-ACC-PH]Physics [physics]/Physics [physics]/Accelerator Physics [physics.acc-ph]7. Clean energy01 natural sciencesNuclear physicsneutrino0103 physical sciencesEmmaFysiklcsh:Nuclear and particle physics. Atomic energy. Radioactivityddc:530010306 general physicsNeutrino oscillationQCAstroparticle physicsPhysicsLarge Hadron ColliderBeta-Beam010308 nuclear & particles physicsFísicaSurfaces and InterfacesAccelerators and Storage RingsNeutrino detectorPhysical Scienceslcsh:QC770-798Physics::Accelerator PhysicsNeutrino FactoryHigh Energy Physics::ExperimentNeutrino[PHYS.ASTR]Physics [physics]/Astrophysics [astro-ph]Storage ringLepton
researchProduct

Intrinsic linearity of bakelite Resistive Plate Chambers operated in streamer mode

2019

Abstract Resistive Plate Chambers have largely been used in High Energy Physics and Cosmic Ray research. In view of using this detector for calorimetry applications it is important to know the maximum measurable particle density, or its intrinsic linearity limit, which is tightly related to the dimension of the discharge region. In this paper we report the results of measurements performed at the Beam Test Facility (INFN National Laboratory of Frascati, Italy) where the intrinsic linearity of bakelite RPCs operated in streamer mode has been tested at different impinging particle densities.

Nuclear and High Energy PhysicsPhysics::Instrumentation and DetectorsIntrinsic linearityStreamer modeCosmic rayCalorimetry01 natural scienceschemistry.chemical_compoundOptics0103 physical sciencesBakeliteParticle density010303 astronomy & astrophysicsInstrumentationPhysicsResistive touchscreen010308 nuclear & particles physicsbusiness.industryDetectorSettore FIS/01 - Fisica SperimentaleLinearityRPC detector Streamer mode Intrinsic linearity CalorimetrychemistryParticlePhysics::Accelerator PhysicsRPC detectorCalorimetry; Intrinsic linearity; RPC detector; Streamer modebusinessBeam (structure)
researchProduct

Comparison of large-angle production of charged pions with incident protons on cylindrical long and short targets

2009

The HARP Collaboration has presented measurements of the double-differential pi(+/-) production cross section in the range of momentum 100 MeV/c <= p <= 800 MeV/c and angle 0.35 rad <=theta <= 2.15 rad with proton beams hitting thin nuclear targets. In many applications the extrapolation to long targets is necessary. In this article the analysis of data taken with long (one interaction length) solid cylindrical targets made of carbon, tantalum, and lead is presented. The data were taken with the large-acceptance HARP detector in the T9 beam line of the CERN proton synchrotron. The secondary pions were produced by beams of protons with momenta of 5, 8, and 12GeV/c. The tracking and identific…

Nuclear and High Energy PhysicsPhysics::Instrumentation and DetectorsNuclear TheoryFOS: Physical sciencesddc:500.27. Clean energy01 natural sciencesBildungHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Basic research0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsNuclear ExperimentPhysics010308 nuclear & particles physicsFísicaSettore FIS/07 - Fisica Applicata(Beni Culturali Ambientali Biol.e Medicin)Calculation methodsResearch councilPhysics::Accelerator PhysicsAngular dependenceHumanitiesParticle Physics - Experiment
researchProduct

The upgraded DO detector

2006

The DØ experiment enjoyed a very successful data-collection run at the Fermilab Tevatron collider between 1992 and 1996. Since then, the detector has been upgraded to take advantage of improvements to the Tevatron and to enhance its physics capabilities. We describe the new elements of the detector, including the silicon microstrip tracker, central fiber tracker, solenoidal magnet, preshower detectors, forward muon detector, and forward proton detector. The uranium/liquid-argon calorimeters and central muon detector, remaining from Run I, are discussed briefly. We also present the associated electronics, triggering, and data acquisition systems, along with the design and implementation of s…

Nuclear and High Energy PhysicsPhysics::Instrumentation and DetectorsTevatron01 natural sciencesParticle detectorlaw.inventionNuclear physicsData acquisitionlaw0103 physical sciencesFermilab010306 general physicsColliderInstrumentationPhysics010308 nuclear & particles physicsbusiness.industryDetectorElectrical engineeringParticle acceleratorD0 experimentExperimental High Energy PhysicsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGPhysics::Accelerator PhysicsHigh Energy Physics::Experimentbusiness
researchProduct

Conceptual design of the AGATA 1$\pi$ array at GANIL

2017

The Advanced GAmma Tracking Array (AGATA) has been installed at the GANIL facility, Caen-France. This setup exploits the stable and radioactive heavy-ions beams delivered by the cyclotron accelerator complex of GANIL. Additionally, it benefits from a large palette of ancillary detectors and spectrometers to address in-beam γ-ray spectroscopy of exotic nuclei. The set-up has been designed to couple AGATA with a magnetic spectrometer, charged-particle and neutron detectors, scintillators for the detection of high-energy γ rays and other devices such as a plunger to measure nuclear lifetimes. In this paper, the design and the mechanical characteristics of the set-up are described. Based on sim…

Nuclear and High Energy PhysicsPlunger devicePhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaCyclotronScintillator[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Accelerator Physics and InstrumentationTracking (particle physics)01 natural sciences7. Clean energylaw.inventionNuclear physicsConceptual designlaw0103 physical sciencesPARIS LaBr3 detectorNeutron detectionPulse shape analysisAGATA spectrometer010306 general physicsNuclear ExperimentInstrumentationPhysicsSpectrometerVAMOS plus plus spectrometer010308 nuclear & particles physicsDetectorFATIMA LaBr3 detectorAcceleratorfysik och instrumenteringDIAMANT detectorNEDA detectorAuthor Keywords:AGATA spectrometerPhysics::Accelerator PhysicsAGATAgamma-ray trackingGANIL facility
researchProduct

The positron distribution in a layered stack sample studied with the use of positron lifetime spectroscopy

2011

Abstract Computer simulation using GEANT4 codes indicates an enhancement of the fraction of implanted positrons stopped in the denser regions of a layered sample. However, positron lifetime measurements performed for layers of pure aluminum, silver and gold foils do not reveal this effect, indicating instead that backscattering plays an important role in determining the positron implantation profile in layered and/or heterogeneous samples.

Nuclear and High Energy PhysicsPositronMaterials sciencechemistryStack (abstract data type)AluminiumPositron Lifetime SpectroscopyPhysics::Accelerator Physicschemistry.chemical_elementAtomic physicsInstrumentationSample (graphics)Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
researchProduct